CN217639613U - Super lens group and optical system comprising same - Google Patents
Super lens group and optical system comprising same Download PDFInfo
- Publication number
- CN217639613U CN217639613U CN202222004007.3U CN202222004007U CN217639613U CN 217639613 U CN217639613 U CN 217639613U CN 202222004007 U CN202222004007 U CN 202222004007U CN 217639613 U CN217639613 U CN 217639613U
- Authority
- CN
- China
- Prior art keywords
- superlens
- group
- super lens
- super
- optical system
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
Images
Landscapes
- Lenses (AREA)
Abstract
The utility model provides a super lens group and contain its optical system, wherein, this method includes: the first super lens, the second super lens, the third super lens and the fourth super lens are sequentially arranged from an object space to an image space; the surfaces of one sides of the substrates of the first super lens, the second super lens, the third super lens and the fourth super lens are provided with nano structures; the nanostructure of each super lens meets the corresponding phase distribution, and the phase distribution corresponding to the four super lenses can enable the super lens group to correct the aberration on the basis of meeting the imaging requirement. Through the embodiment of the utility model provides a super lens group and contain its optical system, based on the super lens group that adopts light in weight that has, small, thickness is thin, the processing degree of difficulty is little and advantages such as low cost, can make image device's such as camera lens that adopt this super lens group TTL reduce, this super lens group is applicable to more and requires among the more strict image device to the TTL more, and whole cost reduction.
Description
Technical Field
The utility model relates to an optical imaging technical field particularly, relates to a super lens group and contain its optical system.
Background
Optical systems have wide applications in our lives, such as mobile phones, cameras, monitoring and the like, which rely on lenses to provide clear image quality. With the development of the semiconductor industry, the volume of a detector chip is smaller and smaller, which also requires that an optical system meets the requirement, and the TTL (Total Track Length) of the optical system is as small as possible.
In order to reduce aberration in a traditional optical system, a plurality of spherical lenses are adopted for realizing, so that the system is long (TTL is large); the performance of several spherical lenses can be realized by one aspherical lens, so that several aspherical lenses are usually adopted for imaging in some devices (such as mobile phones) with strict requirements on system TTL. However, the aspheric lens has high processing difficulty and high cost; in addition, the problem that the weight is heavy and the thickness is thick exists in the traditional glass-based lens group, and the trend of miniaturization development of equipment cannot be well met.
SUMMERY OF THE UTILITY MODEL
In order to solve the above problem, an embodiment of the present invention provides a superlens set and an optical system including the superlens set.
In a first aspect, an embodiment of the present invention provides a superlens set, including: the first super lens, the second super lens, the third super lens and the fourth super lens are sequentially arranged from an object space to an image space; a nanostructure is arranged on one side surface of each substrate of the first superlens, the second superlens, the third superlens and the fourth superlens; the nanostructure of each superlens meets corresponding phase distribution, and the phase distribution corresponding to the four superlenses can enable the superlens group to correct aberration on the basis of meeting imaging requirements.
Optionally, the phase distribution of the nanostructures of each superlens satisfies one of the following formulas:
wherein r representsThe distance from the center of the superlens to any nanostructure on the surface of the superlens; λ represents the operating wavelength of the superlens;
representing a phase associated with the operating wavelength; (x, y) represents the coordinates of the nanostructure on the corresponding superlens; f represents the focal length of the superlens; a is i And b i Both represent real coefficients.
Optionally, the nanostructure material has an extinction coefficient to the operating band of less than 0.01.
Optionally, the nanostructured material comprises fused silica, quartz glass, crown glass, flint glass, sapphire, crystalline silicon, amorphous silicon, or hydrogenated amorphous silicon.
Optionally, the material of the substrate of each superlens comprises fused silica, quartz glass, crown glass, flint glass, sapphire, or alkali glass.
Optionally, the nanostructure of each superlens is different from the material of the substrate.
Optionally, the operating band of the superlens group comprises a near infrared band.
Optionally, the first superlens, the second superlens, and the fourth superlens have positive optical power; the third superlens has a negative optical power.
Optionally, the superlens group further satisfies:
F/D≤1.3；
15°≤HFOV≤39°；
4.23≤f 1 /F≤7.15；
0.69≤f 2 /F≤1.78；
-5.054≤f 3 /F≤-1.53；
0.57≤f 4 /F≤1.41；
wherein F represents an equivalent focal length of the superlens group; d represents the entrance pupil diameter of the superlens group; HFOV represents a maximum half field angle of the superlens group; f. of 1 Represents a focal length of the first superlens; f. of 2 Represents a focal length of the second superlens; f. of 3 Indicating the third hyperpenetrationThe focal length of the mirror; f. of 4 Represents the focal length of the fourth superlens.
Optionally, the superlens group further satisfies: TTL/ImgH is more than or equal to 1.25 and less than or equal to 1.81; wherein TTL represents the total system length of the super lens group; imgH represents the maximum imaging half-width of the superlens group.
Optionally, the superlens group further satisfies:
0.05mm≤d i ≤2mm；
1.5≤n i ≤1.6；
wherein d is i Denotes the thickness, n, of each superlens i Representing the equivalent refractive index of each superlens.
In a second aspect, the embodiments of the present invention further provide an optical system, including: a superlens group and a filter as described in any of the above; the filter plate is arranged on the light emergent side of the super lens group.
The embodiment of the utility model provides an in the above-mentioned scheme that the first aspect provided, the super lens group of adoption has advantages such as light in weight, small, thickness is thin, the processing degree of difficulty is little and low-cost, can make image device's such as camera lens that adopt this super lens group TTL reduce, and this super lens group is applicable to more in requiring stricter equipment (like the cell-phone) to the TTL more.
In the embodiment of the present invention, since the super-lens set is used for imaging, TTL is smaller, and the overall thickness is further reduced; in addition, the adopted super lens group is simple in processing mode, so that an optical system comprising the super lens group is simple in processing, and the cost is greatly reduced; in addition, the super lens group has better correction effect on aberration.
In order to make the aforementioned and other objects, features and advantages of the present invention comprehensible, preferred embodiments accompanied with figures are described in detail below.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below, it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to these drawings without creative efforts.
Fig. 1 is a schematic structural diagram of a superlens group according to an embodiment of the present invention;
fig. 2 is a schematic structural diagram of an optical system according to an embodiment of the present invention;
fig. 3 shows a schematic structural diagram of an optical system provided in embodiment 1;
FIG. 4 is a schematic diagram showing a phase distribution of each superlens in example 1;
FIG. 5 is a view showing the curvature of field and distortion of the optical system in example 1;
FIG. 6 is a diagram showing a modulation transfer function of an optical system in example 1;
fig. 7 is a schematic structural view showing an optical system provided in embodiment 2;
FIG. 8 is a graph showing curvature of field and distortion of an optical system in example 2;
fig. 9 shows a modulation transfer function diagram of an optical system in embodiment 2.
Icon:
1-super lens group, 2-filter, 11-first super lens, 12-second super lens, 13-third super lens and 14-fourth super lens.
Detailed Description
In the description of the present invention, it is to be understood that the terms "center", "longitudinal", "lateral", "length", "width", "thickness", "upper", "lower", "front", "rear", "left", "right", "vertical", "horizontal", "top", "bottom", "inner", "outer", "clockwise", "counterclockwise", and the like indicate orientations or positional relationships based on the orientations or positional relationships shown in the drawings, and are only for convenience of description and simplification of the description, but do not indicate or imply that the device or element referred to must have a particular orientation, be constructed and operated in a particular orientation, and therefore, should not be construed as limiting the present invention.
Furthermore, the terms "first", "second" and "first" are used for descriptive purposes only and are not to be construed as indicating or implying relative importance or implicitly indicating the number of technical features indicated. Thus, a feature defined as "first" or "second" may explicitly or implicitly include one or more of that feature. In the description of the present invention, "a plurality" means two or more unless specifically limited otherwise.
In the present invention, unless otherwise expressly specified or limited, the terms "mounted," "connected," and "fixed" are to be construed broadly and may, for example, be fixedly connected, detachably connected, or integrally connected; can be mechanically or electrically connected; they may be connected directly or indirectly through intervening media, or they may be interconnected between two elements. The specific meaning of the above terms in the present invention can be understood according to specific situations by those skilled in the art.
The embodiment of the utility model provides a super lens assembly, it is shown with reference to fig. 1, this super lens assembly includes: a first superlens 11, a second superlens 12, a third superlens 13 and a fourth superlens 14 which are arranged in sequence from an object space to an image space; FIG. 1 shows the object side on the left side of the superlens group and the image side on the right side of the superlens group.
As shown in fig. 1, one side surface of each of the substrates of the first superlens 11, the second superlens 12, the third superlens 13, and the fourth superlens 14 is provided with a nanostructure; the nanostructure of each super lens meets the corresponding phase distribution, and the phase distribution corresponding to the four super lenses can enable the super lens group to correct the aberration on the basis of meeting the imaging requirement.
The number of the nano structures is multiple, and the nano structures can be arranged in an array form. In the embodiment of the present invention, in order to distinguish the side provided with the nanostructure from the side not provided with the nanostructure, two sides of each superlens may be named, for example, the left side surface of the first superlens 11 may be referred to as a first side, and the right side surface of the first superlens 11 may be referred to as a second side; a left side surface of the second superlens 12 is referred to as a third surface, and a right side surface of the second superlens 12 is referred to as a fourth surface; a left side surface of the third super lens 13 is referred to as a fifth surface, and a right side surface of the third super lens 13 is referred to as a sixth surface; a left side surface of the fourth super lens 14 is referred to as a seventh surface, and a right side surface of the fourth super lens 14 is referred to as an eighth surface. As shown in fig. 1, the nano structures arranged in an array may be disposed on the second surface, the third surface, the sixth surface, and the eighth surface, respectively.
The embodiment of the utility model provides an in, the nanostructure of every super lens can make corresponding super lens have certain phase distribution, and the incident light passes through these four super lenses in proper order, can be carried out quartic phase modulation by these four super lenses in proper order (if carry out phase modulation based on the phase distribution that every super lens corresponds) for this incident light finally can be when generating the image, corrects it and sees through the produced aberration of different super lenses.
The embodiment of the utility model provides an adopted super lens group have light in weight, small, thickness is thin, the processing degree of difficulty is little and advantages such as low cost, can make imaging device's such as the camera lens that adopts this super lens group TTL (system total length) less, should surpass the lens group and be applicable to more strict imaging device (like the cell-phone) to the TTL requirement more in being applicable to.
Optionally, the phase distribution of the nanostructures of each superlens satisfies one of the following formulas:
wherein r represents the distance from the center of the superlens to any nanostructure on the surface of the superlens; λ represents the operating wavelength of the superlens;
representing a phase associated with the operating wavelength; (x, y) represents the coordinates of the nanostructure on the corresponding superlens; f represents the focal length of the superlens; a is i And b i Both represent real coefficients.
In the embodiment of the present invention, the phase distribution of four super lenses (i.e. the first super lens 11, the second super lens 12, the third super lens 13 and the fourth super lens 14) can be expressed by high-order polynomials, and the high-order polynomials include odd-order polynomial and even-order polynomial. In order not to destroy the rotational symmetry of the phase distribution of each superlens, the phase corresponding to the even-order polynomial can be optimized, which greatly reduces the degree of freedom of designing the superlens. In the 8 formulas (1-1) to (1-8), compared with the other formulas (1-4) to (1-6), the phases meeting the odd polynomial can be optimized without destroying the rotational symmetry of the phase distribution of the superlens, so that the optimization degree of freedom of the superlens is greatly improved.
Specifically, the phase distributions corresponding to the first superlens 11, the second superlens 12, the third superlens 13, and the fourth superlens 14 may satisfy any one of the eight formulas, for example, the phase distribution of the first superlens 11 may satisfy the formula (1-1); the phase distribution of the second superlens 12 may satisfy the above formula (1-2); the phase distribution of the third superlens 13 may satisfy the above-mentioned formula (1-3); the phase distribution of the fourth superlens 14 may satisfy the above formula (1-4); the four phase distribution equations may be four different equations; or the phase distribution formula satisfied by each superlens may also be the same, for example, under the condition that the phase distribution formula satisfied by each superlens is the same, the phase coefficient corresponding to each superlens may be changed, and different phase distributions (such as a regulation function) are realized by using different phase coefficients; this embodiment is not limited to this.
Optionally, the nanostructure material has an extinction coefficient to the operating band of less than 0.01. The extinction coefficient of the material of the nano structure arranged on the surface of one side of each super lens to a working waveband is smaller (for example, less than 0.01), the amplitude attenuation of incident light is slower, the more light energy enters the nano structure, and the higher the transmittance of the nano structure is; i.e. the nanostructure material is a material having a high transmittance for the operating band, e.g. the nanostructure is transparent in the operating band. Optionally, the operating band of the superlens group comprises a near infrared band; for example, the incident light to the superlens group may be near-infrared light, i.e., electromagnetic waves between visible light and mid-infrared light, and the near-infrared band may be electromagnetic waves having a wavelength in a range of 780nm to 2526 nm.
Alternatively, the nanostructured material may include: fused quartz, quartz glass, crown glass, flint glass, sapphire, crystalline silicon, amorphous silicon, or hydrogenated amorphous silicon; alternatively, the material of the substrate of each superlens may include: fused quartz, quartz glass, crown glass, flint glass, sapphire, or alkali glass; optionally, the nanostructure of each superlens is different from the material of the substrate. In the embodiment of the present invention, the material of the nano structure of each superlens is different from the material of the substrate for setting the nano structure, for example, the material of the nano structure of the first superlens 11 can be selected from the crystalline silicon, and the material of the substrate of the first superlens 11 can be selected from the quartz glass, which are different from each other.
Optionally, the first superlens 11, the second superlens 12, and the fourth superlens 14 have positive optical power; the third superlens 13 has a negative power.
Wherein, the focal power is used for representing the refractive power (refractive index) of the optical system to the incident parallel light beams, and the focal power of the super lens is equal to the reciprocal of the focal length; positive focal power means that the refractive index of the superlens calculated by the gauss optical theory is positive (the reciprocal of the focal length is positive); negative optical power means that the refractive index of the superlens calculated by the gauss theory is negative (the reciprocal of the focal length is negative). In the embodiment of the present invention, the positive and negative of the focal power corresponding to the four super lenses can be different, for example, the first super lens 11, the second super lens 12 and the fourth super lens 14 have positive focal power, and the third super lens 13 has negative focal power, so as to realize better imaging and aberration correction.
Optionally, the superlens group further satisfies:
F/D≤1.3 (2-1)；
15°≤HFOV≤39° (2-2)；
4.23≤f 1 /F≤7.15 (2-3)；
0.69≤f 2 /F≤1.78 (2-4)；
-5.054≤f 3 /F≤-1.53 (2-5)；
0.57≤f 4 /F≤1.41 (2-6)；
wherein, F represents the Equivalent Focal Length (EFL) of the super lens group; d represents the entrance pupil diameter of the superlens group; F/D represents the ratio of the equivalent focal length of the super lens group to the diameter of the entrance pupil; HFOV (Half Field of View) represents the maximum Half Field angle of the superlens group, i.e., the hyper-transilluminationHalf of the maximum field angle of the lens group; f. of 1 Denotes the focal length of the first superlens 11; f. of 2 Denotes the focal length of the second superlens 12; f. of 3 Denotes the focal length of the third superlens 13; f. of 4 Denotes the focal length of the fourth superlens 14; the above relations (2-3) to (2-6) respectively define the ratio relation between the focal length of each superlens and the equivalent focal length F of the superlens group; when the super lens group satisfies the 6 relations (2-1) to (2-6), the super lens group has better effects on image formation and aberration correction.
Optionally, the superlens group further satisfies: TTL/ImgH is more than or equal to 1.25 and less than or equal to 1.81; wherein, TTL represents the total system length of the super lens group; imgH denotes the maximum imaging half-width of the superlens group.
Wherein TTL represents a Total Tracking Length of the superlens group, for example, a distance from a first surface of a first superlens 11 (a left side surface of the first superlens 11 shown in fig. 1) to an image plane in the superlens group; the ImgH represents a half-height width of the Image plane of the superlens group, i.e., a half of a maximum imaging height (Image High), which is a distance from a point where peripheral field rays converge on the Image plane to the center of the Image plane.
Optionally, the superlens group further satisfies:
0.05mm≤d i ≤2mm；
1.5≤n i ≤1.6；
wherein d is i The thickness of each super lens is expressed, namely the distance between two side surfaces of each super lens; i =1, 2, 3 or 4 e.g. d 1 Represents the thickness of the first superlens 11, such as the distance between the first and second faces of the first superlens 11 in fig. 1; n is a radical of an alkyl radical i Representing the equivalent refractive index of each superlens.
The embodiment of the utility model provides an optical system is still provided, see fig. 2 and show, this optical system includes: the superlens group 1 and the filter 2; the filter 2 is arranged on the light-emitting side of the super lens group 1; fig. 2 shows the superlens group 1 with its light exit side on the right side.
As shown in fig. 2, can set up filter 2 between the light-emitting side of superlens group 1 and image plane, this filter 2 can be near-infrared filter (Nir filter), and this filter 2 can filter the light outside the operating wavelength, only sees through the light of operating wavelength, is favorable to improving the imaging quality of this optical system at near-infrared wave band (operating wavelength).
In the optical system provided by the embodiment of the utility model, the super lens group 1 is adopted for imaging, the TTL is smaller, and the overall thickness is further reduced; in addition, the adopted machining mode of the super lens group 1 is simple, so that the machining of an optical system comprising the super lens group is simple, and the cost is greatly reduced; in addition, the super lens group 1 has a good effect of correcting aberrations.
Example 1:
as shown in fig. 3, this embodiment 1 provides a four-piece superlens-based optical system, in which nanostructures are respectively located on a second face (a right side face of the first superlens 11 in fig. 3), a third face (a left side face of the second superlens 12 in fig. 3), a sixth face (a right side face of the third superlens 13 in fig. 3), and an eighth face (a right side face of the fourth superlens 14 in fig. 3) of the four-piece superlens. In this embodiment 1, the phase distributions of the four superlenses respectively satisfy any one of the above formulas (1-1) to (1-8), and a schematic diagram of the phase distribution of each superlens can be seen in fig. 4.
Specifically, specific parameters of the optical system used in this embodiment 1 can be found in table 1 below:
| content providing method and apparatus | Parameter(s) |
| Working band (WL) | Near infrared band (920 nm-960 nm) |
| Equivalent Focal Length (EFL) | 2.5mm |
| Half field angle (omega) | 39° |
| F number | 1.3 |
| Back Focal Length (BFL) | 1.516mm |
| Total system length (TTL) | 3.8mm |
TABLE 1
Specific parameters of the surfaces of the optical system employed in this example 1 are shown in the following table 2:
TABLE 2
In table 2, surface numbers sequentially represent first to tenth surfaces, wherein numbers 1 to 8 represent two side surfaces of four superlenses, respectively; numbers 9 to 10 indicate two side faces of the filter 2 in the optical system; number 11 denotes an image plane; the standard plane refers to the surface without the nano-structure; a super surface then means a surface with nanostructures. The thicknesses of the first surface, the third surface, the fifth surface and the seventh surface respectively represent the distances from the light-incident side surfaces of the first superlens 11, the second superlens 12, the third superlens 13 and the fourth superlens 14 to the light-emergent side surfaces, namely the thicknesses of the corresponding superlenses; the thicknesses of the second surface, the fourth surface, the sixth surface and the eighth surface respectively represent the distance between the light-emitting side surfaces of the first superlens 11, the second superlens 12, the third superlens 13 and the fourth superlens 14 and the distance between the next superlens; the thickness of the ninth plane refers to the thickness of the filter 2 itself, and the thickness of the tenth plane refers to the distance (i.e., back intercept, BFL) from the filter 2 to the image plane (eleventh plane).
Fig. 5 shows a field curvature and distortion diagram of the optical system provided in the present embodiment 1; fig. 6 shows a Modulation Transfer Function (MTF) diagram of the optical system provided in this embodiment 1. As can be seen from fig. 5 (left part), the field curvature of the optical system is small, i.e., less than 0.1mm; as can be seen from fig. 5 (right part), the distortion of the optical system is less than 2%, e.g., the optical maximum distortion is-1.6%; as can be seen from fig. 6, the modulation transfer functions of the optical system at different fields of view are close to the diffraction limit, for example, the maximum field of view is greater than 30%. In summary, the optical system provided in this embodiment 1 has good imaging performance and excellent astigmatism and curvature of field control.
Example 2:
as shown in fig. 7, the present embodiment 2 provides a four-piece superlens-based optical system, in which the nanostructures are respectively located on a first face (a left face of the first superlens 11 in fig. 7), a fourth face (a right face of the second superlens 12 in fig. 7), a fifth face (a left face of the third superlens 13 in fig. 7), and a seventh face (a left face of the fourth superlens 14 in fig. 7) of the four pieces of superlenses. In embodiment 2, the phase distributions of the four superlenses respectively satisfy any one of the above-described formulas (1-1) to (1-8).
Specifically, the specific parameters of the optical system used in this embodiment 2 can be seen from the following table 3:
| content providing method and apparatus | Parameter(s) |
| Working band (WL) | Near infrared band (920-960 nm) |
| Equivalent Focal Length (EFL) | 0.99mm |
| Half field angle (omega) | 39° |
| F number | 1.1 |
| Back Focal Length (BFL) | 0.71mm |
| Total System Length (TTL) | 2.82mm |
TABLE 3
Specific parameters of the surfaces of the optical system employed in this example 2 are shown in the following table 4:
TABLE 4
Fig. 8 shows a field curvature and distortion diagram of the optical system provided in the present embodiment 2; fig. 9 shows the modulation transfer function of the optical system provided in this embodiment 2. As can be seen from fig. 8 (left part), the field curvature of the optical system is small, i.e., less than 0.8 μm; as can be seen from fig. 8 (right part), the distortion of the optical system is less than 20%; as can be seen from fig. 9, the modulation transfer functions of the optical system at different fields of view are all close to the diffraction limit. In summary, the optical system provided in this embodiment 2 has good imaging performance and excellent control of astigmatism and field curvature.
The above description is only for the specific embodiments of the present invention, but the protection scope of the present invention is not limited thereto, and any person skilled in the art can easily think of the technical solutions of the changes or replacements within the technical scope of the present invention, and all should be covered within the protection scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the claims.
Claims (12)
1. A superlens group, comprising: a first super lens (11), a second super lens (12), a third super lens (13) and a fourth super lens (14) which are arranged in sequence from an object space to an image space;
one side surface of each substrate of the first super lens (11), the second super lens (12), the third super lens (13) and the fourth super lens (14) is provided with a nano structure; the nanostructure of each superlens meets corresponding phase distribution, and the phase distribution corresponding to the four superlenses can enable the superlens group to correct aberration on the basis of meeting imaging requirements.
2. A superlens group according to claim 1, wherein the phase distribution of the nanostructures of each superlens satisfies one of the following formulas:
wherein r represents the distance from the center of the superlens to any nanostructure on the surface of the superlens; λ represents the operating wavelength of the superlens;
representing a phase associated with the operating wavelength; (x, y) represents the coordinates of the nanostructure on the corresponding superlens; f represents the focal length of the superlens; a is i And b i Both represent real coefficients.
3. A superlens group according to claim 1, wherein the nanostructure material has an extinction coefficient to the operating wavelength band of less than 0.01.
4. A superlens group according to claim 3, wherein the nanostructured material comprises fused silica, quartz glass, crown glass, flint glass, sapphire, crystalline silicon, amorphous silicon or hydrogenated amorphous silicon.
5. The superlens group of claim 1, wherein the material of the substrate of each superlens comprises fused silica, quartz glass, crown glass, flint glass, sapphire, or alkali glass.
6. A superlens group according to claim 1, wherein the nanostructure of each superlens is different from the material of the substrate.
7. The superlens group of claim 1, wherein the operating wavelength band of the superlens group includes a near infrared wavelength band.
8. The superlens group of claim 1, wherein the first superlens (11), the second superlens (12) and the fourth superlens (14) have positive optical power; the third superlens (13) has a negative power.
9. The superlens group of claim 8, further satisfying:
F/D≤1.3；
15°≤HFOV≤39°；
4.23≤f 1 /F≤7.15；
0.69≤f 2 /F≤1.78；
-5.054≤f 3 /F≤-1.53；
0.57≤f 4 /F≤1.41；
wherein F represents an equivalent focal length of the superlens group; d represents the entrance pupil diameter of the superlens group; HFOV represents a maximum half field angle of the superlens group; f. of 1 Represents the focal length of the first superlens (11); f. of 2 Represents the focal length of the second superlens (12); f. of 3 Represents the focal length of the third superlens (13); f. of 4 Represents the focal length of the fourth superlens (14).
10. The superlens group of claim 1, further satisfying: TTL/ImgH is more than or equal to 1.25 and less than or equal to 1.81;
wherein TTL represents the total system length of the super lens group; imgH represents the maximum imaging half-width of the superlens group.
11. The superlens group of claim 1, further satisfying:
0.05mm≤d i ≤2mm；
1.5≤n i ≤1.6；
wherein d is i Denotes the thickness of each superlens, n i Representing the equivalent refractive index of each superlens.
12. An optical system, comprising: the superlens group (1) and the filter plate (2) of any of claims 1-11; the filter plate (2) is arranged on the light-emitting side of the super lens assembly (1).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202222004007.3U CN217639613U (en) | 2022-08-01 | 2022-08-01 | Super lens group and optical system comprising same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202222004007.3U CN217639613U (en) | 2022-08-01 | 2022-08-01 | Super lens group and optical system comprising same |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN217639613U true CN217639613U (en) | 2022-10-21 |
Family
ID=83636221
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202222004007.3U Active CN217639613U (en) | 2022-08-01 | 2022-08-01 | Super lens group and optical system comprising same |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN217639613U (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US11927769B2 (en) | 2022-03-31 | 2024-03-12 | Metalenz, Inc. | Polarization sorting metasurface microlens array device |
| US11978752B2 (en) | 2019-07-26 | 2024-05-07 | Metalenz, Inc. | Aperture-metasurface and hybrid refractive-metasurface imaging systems |
| US11988844B2 (en) | 2017-08-31 | 2024-05-21 | Metalenz, Inc. | Transmissive metasurface lens integration |
| US12140778B2 (en) | 2019-07-02 | 2024-11-12 | Metalenz, Inc. | Metasurfaces for laser speckle reduction |
-
2022
- 2022-08-01 CN CN202222004007.3U patent/CN217639613U/en active Active
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US11988844B2 (en) | 2017-08-31 | 2024-05-21 | Metalenz, Inc. | Transmissive metasurface lens integration |
| US12140778B2 (en) | 2019-07-02 | 2024-11-12 | Metalenz, Inc. | Metasurfaces for laser speckle reduction |
| US11978752B2 (en) | 2019-07-26 | 2024-05-07 | Metalenz, Inc. | Aperture-metasurface and hybrid refractive-metasurface imaging systems |
| US11927769B2 (en) | 2022-03-31 | 2024-03-12 | Metalenz, Inc. | Polarization sorting metasurface microlens array device |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN217639613U (en) | Super lens group and optical system comprising same | |
| TWI437258B (en) | Optical lens assembly for image taking | |
| TWI427354B (en) | Photographing optical lens assembly | |
| CN217821058U (en) | TOF lens and imaging system | |
| TWI629501B (en) | Wide angle imaging lens assembly | |
| US20100232013A1 (en) | Infrared imaging lens system and image capture device having same | |
| CN102955227B (en) | optical lens group for imaging | |
| US8456761B2 (en) | Lens system | |
| CN112711127A (en) | Imaging system, lens module and electronic equipment | |
| KR101118910B1 (en) | Photographic lens optical system | |
| CN107436482B (en) | Turning type telescopic fixed-focus lens and camera device | |
| CN212321961U (en) | Thin optical lens | |
| CN212160213U (en) | Optical imaging lens and electronic device | |
| CN114879349B (en) | Optical image capturing lens assembly | |
| US20230065152A1 (en) | Imaging lens | |
| CN114265184B (en) | Optical lens, camera module and electronic equipment | |
| CN210051954U (en) | Optical lens group | |
| CN210038211U (en) | Optical lens group | |
| CN211402911U (en) | Large-zoom-ratio optical passive semi-athermal zoom optical system | |
| JP2024501102A (en) | Optical systems and head-mounted displays | |
| CN114002832A (en) | Optical system, lens module and electronic equipment | |
| TWI802148B (en) | Imaging lens | |
| CN220305554U (en) | Three-piece type optical system for far infrared band | |
| CN118625506B (en) | Infrared microscope objective lens | |
| CN216248547U (en) | Optical imaging system |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| GR01 | Patent grant | ||
| GR01 | Patent grant |